Dynamic Range Extension of a SPAD Imager Using Non-Uniformity Correction Techniques

Figueras, E. Vilella; Garcı́a, J.F.; Alonso, O.; Diéguez, A.

doi:10.1109/jsen.2016.2522651

Cited by 4 publications

(1 citation statement)

References 14 publications

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“…The PDP decreases for longer wavelengths due to the increasing absorption length of photons than cannot be detected by the SPAD shallow junction. PDP non-uniformity, which may reduce the dynamic range of a SPAD imager [14], was 1.1% (standard deviation) between the pixels in one array for the peak PDP at 5V excess bias.…”

Section: Photon Detection Probabilitymentioning

confidence: 99%

Design and characterization of a p+/n-well SPAD array in 150nm CMOS process

Pancheri

Betta

et al. 2017

Opt. Express

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This paper reports on characterization results of a single-photon avalanche diode (SPAD) array in standard CMOS 150nm technology. The array is composed by 25 (5 × 5) SPADs, based on p/n-well active junction along with a retrograde deep n-well guard ring. The square-shaped SPAD has a 10µm active diameter and 15.6µm pitch size, achieving a 39.9% array fill factor. Characterization results show a good breakdown voltage uniformity (40mV max-min) within each chip and 17mV/°C temperature coefficient. The median DCR is 0.4Hz/µm, and the afterpulsing probability is 0.85% for a dead time of 150ns at 3V excess bias voltage. The peak PDP is 31% at 450nm wavelength and a good uniformity (1.1% standard deviation) is observed for the array at 5V excess bias. The single SPADs exhibit a timing jitter of 52ps (FWHM) and 42ps (FWHM) under a 468-nm and a 831-nm laser, respectively. The crosstalk probability as a function of pixel-to-pixel distance and excess bias voltage is presented, and random telegraph signal (RTS) noise is also discussed in detail.

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Section: Photon Detection Probabilitymentioning

confidence: 99%